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Ch 12 Gases Three reasons for studying gases 1. Some common elements and compounds exist as gases 2. Our atmosphere is gaseous 3. Gas behavior is easy to understand at the molecular level, using a mathematical model, which works for most gasses.
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Ch 12 Gases

Jan 17, 2016

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Ch 12 Gases. Three reasons for studying gases 1. Some common elements and compounds exist as gases 2. Our atmosphere is gaseous 3. Gas behavior is easy to understand at the molecular level, using a mathematical model, which works for most gasses. Properties of gases. - PowerPoint PPT Presentation
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Page 1: Ch 12 Gases

Ch 12 Gases

Three reasons for studying gases 1. Some common elements and

compounds exist as gases 2. Our atmosphere is gaseous 3. Gas behavior is easy to understand at

the molecular level, using a mathematical model, which works for most gasses.

Page 2: Ch 12 Gases

Properties of gases Gases can be described using four

quantities

P, V, T (in K) and n (moles)

Page 3: Ch 12 Gases

Gas PressureA tube is filled with mercury. The tube is

inverted into a dish containing mercury. The mercury assumes a level in the tube such that the pressure exerted by the mass of the column of mercury in the tube is balanced by the pressure of the atmosphere pressing down on the surface of the mercury in the dish.

At seal lever, the mercury-filled barometer will rise a760 mmHg in the tube. This unit is sometimes called the torr for Torricelli inventor of the barometer

Page 4: Ch 12 Gases

Gas Pressure

This Galileo thermometer combines art with science. It provides an accurate reading of current weather conditions. Temperature is indicated by the lowest "floating" sphere in the top grouping. As accurate as laboratory thermometers. Predict changes in the weather by referencing fluid rise and fall in the barometric tube. The hygrometer measures humidity. How the thermometer works:The colored floating spheres are "pushed" either up or down depending on the changing density of the clear fluid inside the glass thermometer body. When the temperature goes up, the clear fluid becomes less dense and rises - forcing the spheres down one by one. When the temperature goes down, the clear fluid becomes denser - forcing the spheres upward. 

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Page 5: Ch 12 Gases

Gas Pressure

How the barometer works:While not as accurate as modern day aneroid barometers, the principle of the early "Water Barometer" is sound. When atmospheric pressure decreases, the fluid is pulled upward toward the top of the barometer tube (low pressure). As atmospheric pressure increases, the fluid is "pushed down" (high pressure). Standard atmospheric pressure at sea level is 29.92".

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Page 6: Ch 12 Gases

Gas PressureWater-based barometers This concept of

"decreasing atmospheric pressure predicts stormy weather" was invented by Lucien Vidie It consists of a glass container with a sealed body, half filled with water. A narrow spout connects to the body below the water level and rises above the water level, where it is open to the atmosphere. When the air pressure is lower than it was at the time the body was sealed, the water level in the spout will rise above the water level in the body; when the air pressure is higher, the water level in the spout will drop below the water level in the body.

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Page 7: Ch 12 Gases

Gas PressureAn aneroid barometer uses a small,

flexible metal box called an aneroid cell. This aneroid capsule(cell) is made from an alloy of beryllium and copper.[2] The evacuated capsule (or more usually capsules) is prevented from collapsing by a strong spring. Small changes in external air pressure cause the cell to expand or contract. This expansion and contraction drives mechanical levers such that the tiny movements of the capsule are amplified and displayed on the face of the aneroid barometer.

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Page 8: Ch 12 Gases

Gas Pressure

When the pressure gauge is applied to the valve stem of a tire, the pressurized air from the tire rushes in and pushes the piston toward the right. The distance the piston travels is relative to the pressure in the tire. The pressurized air is pushing the piston to the right, and the spring is pushing back

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Page 9: Ch 12 Gases

Gas Pressure

The calibrated rod fits inside the spring. The calibrated rod rides on top of the piston, but the rod and the piston are not connected and there is a fairly tight fit between the rod and the stop. When the piston moves to the right, it pushes the calibrated rod. When the pressure is released, the piston moves back to the left but the rod stays in its maximum position to allow you to read the pressure.

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Page 10: Ch 12 Gases

Units of Gas Pressure

1 standard atmosphere = 1 atm

1 atm = 760 mm Hg

The SI unit of Pressure is the pascal (Pa) Pressure = force / area 1 Pa = 1 newton / meter2 a Pa is small so kPa is used

1 atm = 760 mmHg = 101.3 kPa = 1.013 bar

Page 11: Ch 12 Gases

Units of Gas Pressure

Convert 635 mm Hg into atm and kPa

Rank the following in decreasing order 75 kPa, 250 mm Hg, 0.83 bar, 0.63 atm.

Page 12: Ch 12 Gases

Gas Pressure and Volume

Boyle

dbhs.wvusd.k12.ca.us/webdocs/GasLaw/Gas-Boyle.html

Volume is inversely proportional to Pressure when n and T are constant P V = constant when n and T are constant

P1V1 = P2V2

www.onr.navy.mil/Focus/blowballast/sub/work4.htm

Page 13: Ch 12 Gases

Gas Temperature and Volume

Charles Law

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www.chm.davidson.edu/ChemistryApplets/GasLaws/CharlesLaw.html

Page 14: Ch 12 Gases

Gas Temperature and Volume

Charles Law allows the calculation of absolute 0 or 0 K

Page 15: Ch 12 Gases

Combined Gas Las Combination of Charles and Boyle’s

Law The ratio between the pressure-volume

constant and the temperature of a system remains constant.

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Page 16: Ch 12 Gases

Combined Gas Las Weather balloons http://www.ultimatechase.com/chase_ac

counts/Weather_Balloon_Launch.htm You have a 22 L cylinder of He at a pressure of 150

atm and at 31 oC. How many balloons can you fill, each with a volume of 5.o L, on a day when the atmospheric pressure is 755 mmHg and the temperature is 22 oC?

Page 17: Ch 12 Gases

Avogadro’s Hypothesis

Equal volumes of gases under the same conditions of temperature and pressure have equal numbers of molecules.

Four interrelated quantities can be used to describe a gas: P, V, T, and n. These 4 quantities can be made into a mathematical equation by introducing a proportionality constant now labeled R

R = .082 l . atm mol . K

Page 18: Ch 12 Gases

Ideal Gas Law

http://intro.chem.okstate.edu/1314F00/laboratory/GLP.htm

Page 19: Ch 12 Gases

Ideal Gas Law

R has a different value for each different unit of pressure and the other quantities used. Some values are...

R = 8.314472 m3·Pa·K-1·mol-1

R = 0.08205784 L·atm·K-1·mol-1

R = 62.3637 L·mmHg·K-1·mol-

Page 20: Ch 12 Gases

Ideal Gas Law

The state of an amount of gas is determined by its pressure, volume, and temperature according to the equation:QuickTime™ and aTIFF (Uncompressed) decompressorare needed to see this picture.

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Ideal Gas Law A balloon with 1300 mol of H2 is at

a temperature of 23oC and a pressure of 750 mmHg, what is the volume of the balloon?

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Page 22: Ch 12 Gases

Ideal Gas Law As the amount of substance could be given in mass instead of

moles, sometimes an alternative form of the ideal gas law is useful.

The number of moles (n ) is equal to the mass m() divided by the molar mass (M):

Then, replacing gives:

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Page 23: Ch 12 Gases

Density of a Gas

Given that D = m/V rearrange the equation to solve for the D of a gas

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Divide by V P = m R T Then get only m on one side V M V So D = m = PM V RT

Page 24: Ch 12 Gases

Density of a Gas

Calculate the density of CO2 gas. Is it more or less dense than air.

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Calculating Molar Mass Calculate the molar mass (M) of a compound when a

0.100 g sample exerts a pressure of 70.5 mm Hg in a 250 mL container at 22.3 oC. The empirical formula is CHF2. Calculate the molecular formula.

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Page 26: Ch 12 Gases

Gas Laws and Chemical Reactions

Page 27: Ch 12 Gases

Gas Laws and Chemical Reactions

Use the following reaction to prepare D2.

2 Li(s) + 2 D2O(l) -> 2 LiOD(aq) + D2(g)

Place 0.125 g of Li metal in 15 mL of D2O (d = 1.11 g / mL) . What amount od D2 (in moles) can be prepared? If dry D2 gas is captured in a 1450 mL flask at 22.o oC, what is the pressure of the gas in mm Hg?. D has an atomic mass of 2.0147 g/ mol)

Page 28: Ch 12 Gases

Gas Laws and Chemical Reactions

Write the reaction for the synthesis of ammonia from its elements.

Assume that 355 L of H2 gas at 25oC and 542 mm Hg is combined with excess N2gas. What amount (mol) of NH3 gas can be produced? If this amount of NH3 gas is stored in a 125 -L tank at 25 oC, what is the pressure of the gas?

Page 29: Ch 12 Gases

Gas and Partial Pressures

Dalton’s Law of Partial Pressure

the pressure of each gas in a mixture is called its partial pressure P

the pressure of a mixture of gases is the sum of the partial pressures of the different gases

Ptotal = P1 + P2 + P3…..

http://www.chm.davidson.edu/ChemistryApplets/GasLaws/DaltonsLaw.html

Page 30: Ch 12 Gases

Dalton’s Law of Partial Pressures

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Dalton’s Law of Partial Pressures

Dalton's Law of Partial Pressures states that for a mixture of gases in a container, the total pressure is equal to the sum of the pressures of each gas. The gas that a diver breathes must be maintained at a partial pressure of 0.20 atm of oxygen. More oxygen could poison the diver, and less would lead to suffocation. The total pressure, however, must be equal to the external pressure to avoid collapsing the lungs. So, a special valve is used to equalize the pressure inside the divers lungs with the external pressure by adding helium gas. The valve also maintains oxygen levels by using Dalton's Law.

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Dalton’s Law of Partial Pressures

Page 33: Ch 12 Gases

For mixtures of gases, use the quantity mole fraction, XX is defined as the number of moles of a gas in a mixture divided By the total number of moles of all gasses. For a mixture of gas A and gas B and Gas C is written as follows

Combining the above equation yields the important equation

Dalton’s Law of Partial Pressures

Page 34: Ch 12 Gases

Partial Pressure Problems

Mix 15.o g of C2HBrClF2 with 23.g g of O2

The total P is 855 mm Hg Calculate the P of each gas.

The mixture above is placed in a 5.00 L tank at 25oC. What is the total P? What is the P of each gas?

Page 35: Ch 12 Gases

Kinetic -Molecular Theory Gases are point masses in space. -

particles small compared to the space they occupy.

Particles are in constant random motion All gases, regardless of their

molecular mass, have the same average kinetic energy at the same temperature.

Page 36: Ch 12 Gases

Kinetic -Molecular Theory http://www.bcpl.net/~kdrews/kmt/kmt.ht

ml

http://chemed.chem.purdue.edu/genchem/topicreview/bp/ch4/kinetic4.html

Page 37: Ch 12 Gases

Kinetic -Molecular TheoryThe kinetic energy of a single molecule of mass m is describedBelow where u is the speed of that molecule.

Two important assumptions 1. Not all molecules have the same speed

2. As temp increases, the number of high speed molecules increases.

The avg KE of a sample of gas molecules depends only on T

Page 38: Ch 12 Gases

Kinetic -Molecular TheoryA sample of gas molecules with avg speed u some moleculesHave speed u1 other molecules have u2, therefore

N is the total number of molecules (n1 + n2 …)

Therefore, the avg KE of molecules is related to u2 the avg of The squares of their speeds (called mean square speed) So the avg KE is described below

Page 39: Ch 12 Gases

Kinetic -Molecular Theory

http://chemed.chem.purdue.edu/genchem/topicreview/bp/ch4/kinetic4.html#kinetic

http://www.chm.davidson.edu/ChemistryApplets/KineticMolecularTheory/Maxwell.html

Page 40: Ch 12 Gases

Kinetic -Molecular Theory

Page 41: Ch 12 Gases

Kinetic -Molecular TheoryThis equation relates mass, average speed, and temperatureThe square root of the mean square speed, called theRoot-mean-square, or rms speed. Where T is in KelvinsAnd related to molar mass, M, Called the Maxwell equation where R = 8.3144 J / K . Mol

All gases have the same average KE at the same Temp However, smaller molecules have greater rms speed

Page 42: Ch 12 Gases

Kinetic -Molecular Theory

Page 43: Ch 12 Gases

Graham’s Law of Effusion Diffusion is the mixing of molecules of

two or more gases due to their molecular motions.

Effusion is the movement of gas through a tiny opening in a container into another container.

Page 44: Ch 12 Gases

Graham’s Law of Diffusion

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A molecule of an ideal gas moves from point A to point B. The molecule ignores the other molecules present.It moves in a straight line path until it collides against the wall, bounces off, and continues to travel in a new straight-line path, again, ignoring other molecules that it passes by. It behaves like it is a billiard ball that was hit once on an empty table.Using the expression for the root mean square velocity (v = square root of (3RT/M)), at room temperature, the typical velocity should be about 100 - 1000 m/sec. One finds, however, that measured diffusion rates are much slower than the typical velocities of molecules in an ideal gas.

Page 45: Ch 12 Gases

Graham’s Law of Diffusion

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Diffusion times are longer because the average time between collisions between molecules is very short. These collisions prevent the molecules from traveling in a straight line motion. Thus, it takes longer for one molecule to go from point A to point B.

Page 46: Ch 12 Gases

Graham’s Law of Effusion

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Graham’s Law of Effusion Graham found experimentally that the

rate of effusion of a gas is inversely proportional to the square root of the mass of its particles. QuickTime™ and a

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Rate1 is the rate of effusion of the first gas.Rate2 is the rate of effusion for the second gas.M1 is the molar mass of gas 1M2 is the molar mass of gas 2.

Page 48: Ch 12 Gases

Nonideal Behavior: Real Gases Real Gases: • Are affected by intermolecular

forces of attraction (otherwise, a gas could not become a liquid)

• Undergo non-elastic collisions • Do occupy space These differences between

how a real gas and and ideal gas act are negligible except at high pressures and low temperature. Real Gases

• In the real world, the behavior of gases only conforms to the ideal-gas equation at relatively high temperature and low pressure.

Page 49: Ch 12 Gases

Nonideal Behavior: Real Gases

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Nonideal Behavior: Real Gases

Thus, for real gases, the following should be expected when the volume of the container becomes small that the molecules are forced to be closer to each other:

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Nonideal Behavior: Real Gases

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In real life, condensation occurs.At some point in the PV diagram, the vapor turns into liquid:

Page 52: Ch 12 Gases

Nonideal Behavior: Real Gases

Intermolecular interactions

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Page 53: Ch 12 Gases

Nonideal Behavior: Real Gases

Intermolecular interactions

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excluded volume (molecules take up space)

Page 54: Ch 12 Gases

Nonideal Behavior: Real GasesVan der Waals Equation

van der Waals equation of state:

(P + (n2a/V2)) (V - nb) = nRT

a and b are the van der Waals constants (characteristic of the gas under study)

a corrects for intermolecular interaction, the density (n/V) is included since at higher densities, there should be greater opportunity for intermolecular interactionsb corrects for the volume of each molecule.

Page 55: Ch 12 Gases

Nonideal Behavior: Real GasesVan der Waals Equation

At large V, (n2a/V2) approaches zero. And V-nb approaches V.At low V (high P), the correction factors become important.

Page 56: Ch 12 Gases

Nonideal Behavior: Real GasesVan der Waals Equation

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